矩形格子中中子通量分布的积分输运理论计算

J. Wood, M.M.R. Williams
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引用次数: 6

摘要

在假设单能中子和各向同性散射的情况下,用积分输运理论计算无限矩形晶格中的通量分布。该方法的重要特点是:精确地处理了矩形单元的边界,并明确地包括了周围单元对参考单元的贡献。该方法在计算机程序CELTIC中实现,并描述了该程序用于求解奇异积分方程的数值技术。通过与空间等截面情况下的精确解析结果的比较,评价了CELTIC的收敛性和准确性。用CELTIC计算了众所周知的Thie晶格的通量和不利因素,并与以前使用各种传输技术的工作者得到的结果进行了比较,这些技术大多依赖于圆柱化单元近似。由于在圆柱化单元中使用“白”边界条件而不是反射边界条件而导致精度的增加。研究了在中子截面不变的情况下,随着电池宽度的减小,直到燃料区变成内切圆,不利因子ξ随电池体积/燃料体积比的变化规律。在ξ曲线上找到了一个最小值,这证实了先前论文中所得到的结果,然而,该结果假设方形电池中的中子截面空间恒定。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
An integral transport theory calculation of neutron flux distributions in rectangular lattice cells

An integral transport theory method is described for calculating the flux distribution in an infinite, rectangular lattice, assuming mono-energetic neutrons and isotropic scattering. Important features of the method are: the rectangular cell boundary is treated exactly and the contribution of the surrounding cells to the reference cell is included explicitly.

The method is implemented in a computer program, CELTIC, and a description is given of the numerical techniques used by the program to solve the singular integral equation. The convergence and accuracy of CELTIC is assessed by a comparison with exact analytic results which are obtainable for the spatially constant cross section case.

Fluxes and disadvantage factors for the well-known Thie lattices are computed by CELTIC and compared with the results obtained by previous workers who used various transport techniques most of which rely on the cylindricalized cell approximation. The increase in accuracy resulting from the use of ‘White’ boundary conditions rather than the reflecting boundary condition in the cylindricalized cell is demonstrated.

The variation of the disadvantage factor, ξ, as a function of the cell volume/fuel volume ratio is studied as the cell width decreases until the fuel region becomes the inscribed circle, for the case that the neutron cross sections remain unchanged. A minimum in the ξ curve is found, which confirms the result obtained in a previous paper which, however, assumed spatially constant neutron cross sections in the square cell.

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